Abstract
Networks play an important role in electrical and electronic engineering. It depends on what area of electrical and electronic engineering, for example there is a lot more abstract mathematics in communication theory and signal processing and networking etc. Networks involve nodes communicating with each other. Graph theory has found a considerable use in this area of research. A topological index is a real number associated with chemical constitution purporting for correlation of chemical networks with various physical properties, chemical reactivity. The concept of hyper Zagreb index, first multiple Zagreb index, second multiple Zagreb index and Zagreb polynomials was established in chemical graph theory based on vertex degrees. In this paper, we extend this study to interconnection networks and derive analytical closed results of hyper Zagreb index, first multiple Zagreb index, second multiple Zagreb index, Zagreb polynomials and redefined Zagreb indices for block shift network (BSN − 1) and (BSN − 2), hierarchical hypercube (HHC − 1) and (HHC − 2).
1 Introduction
Multiprocessor interconnection networks are often required to connect thousands of homogeneously replicated processor-memory pairs, each of which is called a processing node. Instead of using a shared memory, all synchronization and communication between processing nodes for program execution is often done via message passing. Design and use of multi processor interconnection networks have recently drawn considerable attention due to the availability of inexpensive, powerful microprocessors and memory chips. The mesh networks have been recognized as versatile interconnection networks for massively parallel computing. Mesh/torus-like low-dimensional networks have recently received a lot of attention for their better scalability to larger networks, as opposed to more complex networks such as hypercubes. In particular the failure of cooperation on dependent networks has been studied a lot recently in [1].
A number of hierarchical inter connection network (HIN) provide a framework for designing networks with reduced link cost by taking advantage of the locality of communication that exist in parallel applications. HIN employ multiple level. Lower level network provide local communication while higher level networks facilitate remote communication. The multistage networks have long been used as communication networks for parallel computing [2].
The topological properties of certain networks are studied in [3]. Molecules and molecular compounds are often modeled by molecular graphs. A molecular graph is a graph in which vertices are atoms of a given molecule and edges are its chemical bonds. Since the valency of carbon is four, it is natural to consider all graphs with maximum degree ≤ 4, as a molecular graph. A graph G(V, E) with vertex set V and edge set E is connected, if there exists a connection between any pair of vertices in G. A network is simply a connected graph having no multiple edges and no loops. Throughout this article, the degree of a vertex v ∈ V(G), denoted by deg(v), is the number of edges incident to v.
A topological index is a numeric quantity associated with a graph which characterizes the topology of a graph and is invariant under graph automorphism. In more precise way, a topological index Top(G) of a graph G, is a number with the property that for every graph H isomorphic to graph G, Top(H) = Top(G). The concept of topological index came from work done by Wiener [4], while he was working on a boiling point of paraffin. He named this index as the path number. Later on, the path number was renamed as the Wiener index. The Wiener index is the first and the most studied topological index, both from theoretical point of view and applications, and defined as the sum of distances between all pairs of vertices in G, see for details [5, 6].
One of the oldest topological indices is the first Zagreb index introduced by I. Gutman and N.Trinajstic based on degree of vertices of G in 1972 [7]. The first and the second Zagreb indices of a graph G are defined as:
In 2013, G. H. Shirdel, H.R. Pour and A. M. Sayadi [8] introduced a new degree based on Zagreb index named “ hyper Zagreb index" as:
M. Ghorbani and N. Azimi defined two new versions of Zagreb indices of a graph G in 2012 [9]. These indices are the first multiplicative Zagreb index PM1(G) and the second multiplicative Zagreb index PM2(G) and are defined respectively as:
The properties of PM1(G) and PM2(G) indices for some chemical structures have been studied in [10]. The first Zagreb polynomial M1(G, x) and the second Zagreb polynomial M2(G, x) are defined as:
The properties of Zagreb polynomials for some chemical structures have been studied in [11].
Ranjini et al. [12] reclassified the Zagreb indices, to be specific, the redefined first, second and third Zagreb indices for a graph G as;
Nowadays, there is an extensive research activity on HM(G), PM1(G), PM2(G) indices and M1(G, x), M2(G, x) polynomials and their variants, see also [13, 14, 15].
For further study of topological indices of various graph families, see [16, 17, 18, 19, 20, 21, 22, 23, 24, 25, 26, 27, 28, 29, 30].
2 Methods
For the calculation of our outcomes, we used a methodology for combinatorial enlisting, a vertex segment procedure, an edge parcel procedure, diagram theoretical instruments, logical frameworks, a degree-tallying technique, and degrees of neighbors system.
3 Results for block shift network (BSN − 1)n×n
In this section, we compute certain degree based topological indices for block shift network (BSN), see Figure 1(a). The Randic type indices for hierarchical interconnection networks is computed by Haider et. al in [31]. We compute first and second Zagreb indices, hyper Zagreb index HM (G), first multiple Zagreb index PM1(G), second multiple Zagreb index PM2(G) and Zagreb polynomials M1(G, x), M2(G, x) for (BSN − 1)n×n.

(a) block shift network (BSN − 1)3×3 (b) block shift network (BSN − 2)1×1
Let G be a block shift network. The number of vertices and edges in (BSN − 1)n×n is 16n2 and 24n2 − 2, respectively. There are two types of edges in (BSN − 1)n×n based on degrees of end vertices of each edge. The edge set of (BSN − 1)n×n can be divided into two partitions based on the degree of end vertices. The first edge partition E1((BSN −1)n×n) contains 8 edges uv, where deg(u) = 2, deg(v) = 3. The second edge partition E2((BSN − 1)n×n) contains 24n2 − 10 edges uv, where deg(u) = deg(v) = 3.
– The first and second Zagreb indices of (BSN − 1)n×n
Now using Eqs. (1),(2), we have
– Hyper Zagreb index of (BSN − 1)n×n
The hyper Zagreb index using Eq. (3) is computed as:
– Multiplicative Zagreb indices of (BSN − 1)n×n
The multiplicative Zagreb indices using Eqs. (4), (5) are computed as:
– The first and second Zagreb polynomials of (BSN − 1)n×n
Now using Eqs. (6),(7), we have
– The redefined first, second, and third Zegreb index of (BSN − 1)n×n
Now using the edge partition of the block shift network G, and Eq. (8), we have:
By using Eq. (9), the second redefined Zagreb index is computed as below:
Now by using Eq. (10), the third redefined Zagreb index is computed as:
4 Results for block shift network (BSN − 2)n×n
The number of vertices and edges in (BSN −2)n×n are 16n2 and 32n2 − 2 respectively see Figure 1(b). There are two types of edges in (BSN − 2)n×n based on degrees of end vertices of each edge. The edge set of (BSN − 2)n×n can be divided into two partitions based on the degree of end vertices. The first edge partition E1((BSN − 2)n×n) contains 12 edges uv, where deg(u) = 3, deg(v) = 4. The second edge partition E2((BSN − 2)n×n) contains 32n2 − 14 edges uv, where deg(u) = deg(v) = 4.
– The first and second Zagreb indices of (BSN − 2)n×n
Now using Eqs. (1),(2), we have
– Hyper Zagreb index of (BSN − 2)n×n
The hyper Zagreb index using Eq. (3) is computed as:
– Multiplicative Zagreb indices of (BSN − 2)n×n
The multiplicative Zagreb indices using Eqs. (4), (5) are computed as:
– The first and second Zagreb polynomials of (BSN − 2)n×n
Now using Eqs. (6),(7), we have
– The redefined first, second, and third Zegreb index of (BSN − 2)n×n
Now using Eq. (8) and the edge partition of the block shift network (BSN − 2)n×n, we have:
By using Eq. (9), the second redefined Zagreb index is computed as below:
Now by using Eq. (10), the third redefined Zagreb index is computed as:
5 Results for hierarchical hypercube network (HHC − 1)n×n
In this section, we compute certain degree based topological indices of hierarchical interconnection networks see Figure 2(a). The Randic type indices for hierarchical interconnection networks is computed by Haider et. al in [31]. We compute first and second Zagreb indices, hyper Zagreb index HM (G), first multiple Zagreb index PM1(G), second multiple Zagreb index PM2(G) and Zagreb polynomials M1(G, x), M2(G, x) for hierarchical hypercube network (HHC − 1)n×n and hierarchical hypercube network (HHC − 2)n×n.

(a) Hierarchical hypercube network (HHC − 1)1×1 (b) Hierarchical hypercube network (HHC − 2)1×1.
The numbers of vertices and edges in (HHC −1)n×n are 16n + 16 and 24n + 20, respectively. There are two types of edges in (HHC − 1)n×n based on degrees of end vertices of each edge. The edge set of (HHC − 1)n×n can be divided into two partitions based on the degree of end vertices. The first edge partition E1((HHC −1)n×n) contains 16 edges uv, where deg(u) = 2, deg(v) = 3. The second edge partition E2((HHC − 1)n×n) contains 24n + 4 edges uv, where deg(u) = deg(v) = 3.
– The first and second Zagreb indices of (HHC − 1)n×n
Now using Eqs. (1),(2), we have
– Hyper Zagreb index of (HHC − 1)n×n
The hyper Zagreb index using Eq. (3) is computed as:
– Multiple Zagreb indices of (HHC − 1)n×n
The multiple-zagreb indices using Eqs. (4), (5) are computed as:
– The first and second Zagreb polynomials of (HHC − 1)n×n
Now using Eqs. (6),(7), we have
– The redefined first, second, and third Zegreb index of (HHC − 1)n×n
Now using Eq. (8) and the edge partition of the block shift network (HHC − 1)n×n, we have:
By using Eq. (9), the second redefined Zagreb index is computed as below:
Now by using Eq. (10), the third redefined Zagreb index is computed as:
6 Results for hierarchical hypercube network (HHC − 2)n×n
The number of vertices and edges in (HHC−2)n×n are 16n2 and 32n2 − 2, respectively (see Figure 2(b)). There are two types of edges in (HHC − 2)n×n based on degrees of end vertices of each edge. The edge set of (HHC − 2)n×n can be divided into two partitions based on the degree of end vertices. The first edge partition E1((HHC −2)n×n) contains 24 edges uv, where deg(u) = 3, deg(v) = 4. The second edge partition E2((HHC−2)n×n) contains 32n+4 edges uv, where deg(u) = deg(v) = 4.
– The first and second Zagreb indices of (HHC − 2)n×n
Now using Eqs. (1),(2), we have
– Hyper Zagreb index of (HHC − 2)n×n
The hyper Zagreb index using Eq. (3) is computed as:
– Multiple Zagreb indices of (HHC − 2)n×n
The Multiple-Zagreb indices using Eqs. (4), (5) are computed as:
– The first and second Zagreb polynomials of (HHC − 2)n×n
Now using Eqs. (6),(7), we have
– The redefined first, second, and third Zegreb index of (HHC − 2)n×n
Now using Eq. (8) and the edge partition of the block shift network (HHC − 2)n×n, we have:
By using Eq. (9), the second redefined Zagreb index is computed as below:
Now by using Eq. (10), the third redefined Zagreb index is computed as:
Conclusion
In this paper we determined first Zagreb index M1(G), second Zagreb index M2(G), hyper Zagreb index HM(G), first multiple Zagreb index PM1(G), second multiple Zagreb index PM2(G), Zagreb polynomials M1(G, x) and M2(G, x), and redefined Zagreb indices for block shift networks and hierarchical hypercube networks. In future, we are interested in designing some new architectures/ networks and then studying their topological indices which will be quite helpful in understanding their underlying topologies.
Acknowledgement
The authors are grateful to the anonymous referees for their valuable comments and suggestions that improved this paper.
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- Three phase heat and mass transfer model for unsaturated soil freezing process: Part 1 - model development
- Three phase heat and mass transfer model for unsaturated soil freezing process: Part 2 - model validation
- Mathematical model for thermal and entropy analysis of thermal solar collectors by using Maxwell nanofluids with slip conditions, thermal radiation and variable thermal conductivity
- Constructing analytic solutions on the Tricomi equation
- Feynman diagrams and rooted maps
- New type of chaos synchronization in discrete-time systems: the F-M synchronization
- Unsteady flow of fractional Oldroyd-B fluids through rotating annulus
- A note on the uniqueness of 2D elastostatic problems formulated by different types of potential functions
- On the conservation laws and solutions of a (2+1) dimensional KdV-mKdV equation of mathematical physics
- Computational methods and traveling wave solutions for the fourth-order nonlinear Ablowitz-Kaup-Newell-Segur water wave dynamical equation via two methods and its applications
- Siewert solutions of transcendental equations, generalized Lambert functions and physical applications
- Numerical solution of mixed convection flow of an MHD Jeffery fluid over an exponentially stretching sheet in the presence of thermal radiation and chemical reaction
- A new three-dimensional chaotic flow with one stable equilibrium: dynamical properties and complexity analysis
- Dynamics of a dry-rebounding drop: observations, simulations, and modeling
- Modeling the initial mechanical response and yielding behavior of gelled crude oil
- Lie symmetry analysis and conservation laws for the time fractional simplified modified Kawahara equation
- Solitary wave solutions of two KdV-type equations
- Applying industrial tomography to control and optimization flow systems
- Reconstructing time series into a complex network to assess the evolution dynamics of the correlations among energy prices
- An optimal solution for software testing case generation based on particle swarm optimization
- Optimal system, nonlinear self-adjointness and conservation laws for generalized shallow water wave equation
- Alternative methods for solving nonlinear two-point boundary value problems
- Global model simulation of OH production in pulsed-DC atmospheric pressure helium-air plasma jets
- Experimental investigation on optical vortex tweezers for microbubble trapping
- Joint measurements of optical parameters by irradiance scintillation and angle-of-arrival fluctuations
- M-polynomials and topological indices of hex-derived networks
- Generalized convergence analysis of the fractional order systems
- Porous flow characteristics of solution-gas drive in tight oil reservoirs
- Complementary wave solutions for the long-short wave resonance model via the extended trial equation method and the generalized Kudryashov method
- A Note on Koide’s Doubly Special Parametrization of Quark Masses
- On right-angled spherical Artin monoid of type Dn
- Gas flow regimes judgement in nanoporous media by digital core analysis
- 4 + n-dimensional water and waves on four and eleven-dimensional manifolds
- Stabilization and Analytic Approximate Solutions of an Optimal Control Problem
- On the equations of electrodynamics in a flat or curved spacetime and a possible interaction energy
- New prediction method for transient productivity of fractured five-spot patterns in low permeability reservoirs at high water cut stages
- The collinear equilibrium points in the restricted three body problem with triaxial primaries
- Detection of the damage threshold of fused silica components and morphologies of repaired damage sites based on the beam deflection method
- On the bivariate spectral quasi-linearization method for solving the two-dimensional Bratu problem
- Ion acoustic quasi-soliton in an electron-positron-ion plasma with superthermal electrons and positrons
- Analysis of projectile motion in view of conformable derivative
- Computing multiple ABC index and multiple GA index of some grid graphs
- Terahertz pulse imaging: A novel denoising method by combing the ant colony algorithm with the compressive sensing
- Characteristics of microscopic pore-throat structure of tight oil reservoirs in Sichuan Basin measured by rate-controlled mercury injection
- An activity window model for social interaction structure on Twitter
- Transient thermal regime trough the constitutive matrix applied to asynchronous electrical machine using the cell method
- On the zagreb polynomials of benzenoid systems
- Integrability analysis of the partial differential equation describing the classical bond-pricing model of mathematical finance
- The Greek parameters of a continuous arithmetic Asian option pricing model via Laplace Adomian decomposition method
- Quantifying the global solar radiation received in Pietermaritzburg, KwaZulu-Natal to motivate the consumption of solar technologies
- Sturm-Liouville difference equations having Bessel and hydrogen atom potential type
- Study on the response characteristics of oil wells after deep profile control in low permeability fractured reservoirs
- Depiction and analysis of a modified theta shaped double negative metamaterial for satellite application
- An attempt to geometrize electromagnetism
- Structure of traveling wave solutions for some nonlinear models via modified mathematical method
- Thermo-convective instability in a rotating ferromagnetic fluid layer with temperature modulation
- Construction of new solitary wave solutions of generalized Zakharov-Kuznetsov-Benjamin-Bona-Mahony and simplified modified form of Camassa-Holm equations
- Effect of magnetic field and heat source on Upper-convected-maxwell fluid in a porous channel
- Physical cues of biomaterials guide stem cell fate of differentiation: The effect of elasticity of cell culture biomaterials
- Shooting method analysis in wire coating withdrawing from a bath of Oldroyd 8-constant fluid with temperature dependent viscosity
- Rank correlation between centrality metrics in complex networks: an empirical study
- Special Issue: The 18th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering
- Modeling of electric and heat processes in spot resistance welding of cross-wire steel bars
- Dynamic characteristics of triaxial active control magnetic bearing with asymmetric structure
- Design optimization of an axial-field eddy-current magnetic coupling based on magneto-thermal analytical model
- Thermal constitutive matrix applied to asynchronous electrical machine using the cell method
- Temperature distribution around thin electroconductive layers created on composite textile substrates
- Model of the multipolar engine with decreased cogging torque by asymmetrical distribution of the magnets
- Analysis of spatial thermal field in a magnetic bearing
- Use of the mathematical model of the ignition system to analyze the spark discharge, including the destruction of spark plug electrodes
- Assessment of short/long term electric field strength measurements for a pilot district
- Simulation study and experimental results for detection and classification of the transient capacitor inrush current using discrete wavelet transform and artificial intelligence
- Magnetic transmission gear finite element simulation with iron pole hysteresis
- Pulsed excitation terahertz tomography – multiparametric approach
- Low and high frequency model of three phase transformer by frequency response analysis measurement
- Multivariable polynomial fitting of controlled single-phase nonlinear load of input current total harmonic distortion
- Optimal design of a for middle-low-speed maglev trains
- Eddy current modeling in linear and nonlinear multifilamentary composite materials
- The visual attention saliency map for movie retrospection
- AC/DC current ratio in a current superimposition variable flux reluctance machine
- Influence of material uncertainties on the RLC parameters of wound inductors modeled using the finite element method
- Cogging force reduction in linear tubular flux switching permanent-magnet machines
- Modeling hysteresis curves of La(FeCoSi)13 compound near the transition point with the GRUCAD model
- Electro-magneto-hydrodynamic lubrication
- 3-D Electromagnetic field analysis of wireless power transfer system using K computer
- Simplified simulation technique of rotating, induction heated, calender rolls for study of temperature field control
- Design, fabrication and testing of electroadhesive interdigital electrodes
- A method to reduce partial discharges in motor windings fed by PWM inverter
- Reluctance network lumped mechanical & thermal models for the modeling and predesign of concentrated flux synchronous machine
- Special Issue Applications of Nonlinear Dynamics
- Study on dynamic characteristics of silo-stock-foundation interaction system under seismic load
- Microblog topic evolution computing based on LDA algorithm
- Modeling the creep damage effect on the creep crack growth behavior of rotor steel
- Neighborhood condition for all fractional (g, f, n′, m)-critical deleted graphs
- Chinese open information extraction based on DBMCSS in the field of national information resources
- 10.1515/phys-2018-0079
- CPW-fed circularly-polarized antenna array with high front-to-back ratio and low-profile
- Intelligent Monitoring Network Construction based on the utilization of the Internet of things (IoT) in the Metallurgical Coking Process
- Temperature detection technology of power equipment based on Fiber Bragg Grating
- Research on a rotational speed control strategy of the mandrel in a rotary steering system
- Dynamic load balancing algorithm for large data flow in distributed complex networks
- Super-structured photonic crystal fiber Bragg grating biosensor image model based on sparse matrix
- Fractal-based techniques for physiological time series: An updated approach
- Analysis of the Imaging Characteristics of the KB and KBA X-ray Microscopes at Non-coaxial Grazing Incidence
- Application of modified culture Kalman filter in bearing fault diagnosis
- Exact solutions and conservation laws for the modified equal width-Burgers equation
- On topological properties of block shift and hierarchical hypercube networks
- Elastic properties and plane acoustic velocity of cubic Sr2CaMoO6 and Sr2CaWO6 from first-principles calculations
- A note on the transmission feasibility problem in networks
- Ontology learning algorithm using weak functions
- Diagnosis of the power frequency vacuum arc shape based on 2D-PIV
- Parametric simulation analysis and reliability of escalator truss
- A new algorithm for real economy benefit evaluation based on big data analysis
- Synergy analysis of agricultural economic cycle fluctuation based on ant colony algorithm
- Multi-level encryption algorithm for user-related information across social networks
- Multi-target tracking algorithm in intelligent transportation based on wireless sensor network
- Fast recognition method of moving video images based on BP neural networks
- Compressed sensing image restoration algorithm based on improved SURF operator
- Design of load optimal control algorithm for smart grid based on demand response in different scenarios
- Face recognition method based on GA-BP neural network algorithm
- Optimal path selection algorithm for mobile beacons in sensor network under non-dense distribution
- Localization and recognition algorithm for fuzzy anomaly data in big data networks
- Urban road traffic flow control under incidental congestion as a function of accident duration
- Optimization design of reconfiguration algorithm for high voltage power distribution network based on ant colony algorithm
- Feasibility simulation of aseismic structure design for long-span bridges
- Construction of renewable energy supply chain model based on LCA
- The tribological properties study of carbon fabric/ epoxy composites reinforced by nano-TiO2 and MWNTs
- A text-Image feature mapping algorithm based on transfer learning
- Fast recognition algorithm for static traffic sign information
- Topical Issue: Clean Energy: Materials, Processes and Energy Generation
- An investigation of the melting process of RT-35 filled circular thermal energy storage system
- Numerical analysis on the dynamic response of a plate-and-frame membrane humidifier for PEMFC vehicles under various operating conditions
- Energy converting layers for thin-film flexible photovoltaic structures
- Effect of convection heat transfer on thermal energy storage unit